US5504429A - Probe for detecting and dosing molecular oxygen by means of electronic paramagnetic resonance spectrometry - Google Patents
Probe for detecting and dosing molecular oxygen by means of electronic paramagnetic resonance spectrometry Download PDFInfo
- Publication number
 - US5504429A US5504429A US08/114,837 US11483793A US5504429A US 5504429 A US5504429 A US 5504429A US 11483793 A US11483793 A US 11483793A US 5504429 A US5504429 A US 5504429A
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 - chamber
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 - movable magnet
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 - probe according
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Links
- 239000000523 sample Substances 0.000 title claims abstract description 27
 - 230000005298 paramagnetic effect Effects 0.000 title claims abstract description 10
 - MYMOFIZGZYHOMD-UHFFFAOYSA-N Dioxygen Chemical compound O=O MYMOFIZGZYHOMD-UHFFFAOYSA-N 0.000 title claims abstract description 5
 - 229910001882 dioxygen Inorganic materials 0.000 title claims abstract description 5
 - 238000004611 spectroscopical analysis Methods 0.000 title abstract description 4
 - 239000011521 glass Substances 0.000 claims abstract description 19
 - WHXSMMKQMYFTQS-UHFFFAOYSA-N Lithium Chemical compound [Li] WHXSMMKQMYFTQS-UHFFFAOYSA-N 0.000 claims abstract description 18
 - 229910052744 lithium Inorganic materials 0.000 claims abstract description 18
 - 238000004804 winding Methods 0.000 claims abstract description 7
 - IEQIEDJGQAUEQZ-UHFFFAOYSA-N phthalocyanine Chemical compound N1C(N=C2C3=CC=CC=C3C(N=C3C4=CC=CC=C4C(=N4)N3)=N2)=C(C=CC=C2)C2=C1N=C1C2=CC=CC=C2C4=N1 IEQIEDJGQAUEQZ-UHFFFAOYSA-N 0.000 claims abstract 6
 - 230000010287 polarization Effects 0.000 claims description 18
 - 230000005291 magnetic effect Effects 0.000 claims description 13
 - 229910001220 stainless steel Inorganic materials 0.000 claims description 11
 - 239000010935 stainless steel Substances 0.000 claims description 11
 - 230000005284 excitation Effects 0.000 claims description 6
 - 230000005484 gravity Effects 0.000 claims description 3
 - 229910000831 Steel Inorganic materials 0.000 claims 3
 - 239000010959 steel Substances 0.000 claims 3
 - 239000007787 solid Substances 0.000 description 9
 - QVGXLLKOCUKJST-UHFFFAOYSA-N atomic oxygen Chemical compound [O] QVGXLLKOCUKJST-UHFFFAOYSA-N 0.000 description 8
 - 239000001301 oxygen Substances 0.000 description 8
 - 229910052760 oxygen Inorganic materials 0.000 description 8
 - 230000006698 induction Effects 0.000 description 7
 - 238000000034 method Methods 0.000 description 5
 - 238000001514 detection method Methods 0.000 description 4
 - 238000009434 installation Methods 0.000 description 2
 - 238000005259 measurement Methods 0.000 description 2
 - 239000000126 substance Substances 0.000 description 2
 - 238000010521 absorption reaction Methods 0.000 description 1
 - 238000003287 bathing Methods 0.000 description 1
 - 230000015572 biosynthetic process Effects 0.000 description 1
 - 230000008878 coupling Effects 0.000 description 1
 - 238000010168 coupling process Methods 0.000 description 1
 - 238000005859 coupling reaction Methods 0.000 description 1
 - 239000013078 crystal Substances 0.000 description 1
 - 238000009826 distribution Methods 0.000 description 1
 - 239000007789 gas Substances 0.000 description 1
 - 239000008246 gaseous mixture Substances 0.000 description 1
 - 238000004519 manufacturing process Methods 0.000 description 1
 - 230000005311 nuclear magnetism Effects 0.000 description 1
 - 230000003287 optical effect Effects 0.000 description 1
 - 238000003786 synthesis reaction Methods 0.000 description 1
 
Images
Classifications
- 
        
- G—PHYSICS
 - G01—MEASURING; TESTING
 - G01R—MEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
 - G01R33/00—Arrangements or instruments for measuring magnetic variables
 - G01R33/20—Arrangements or instruments for measuring magnetic variables involving magnetic resonance
 - G01R33/28—Details of apparatus provided for in groups G01R33/44 - G01R33/64
 - G01R33/30—Sample handling arrangements, e.g. sample cells, spinning mechanisms
 - G01R33/307—Sample handling arrangements, e.g. sample cells, spinning mechanisms specially adapted for moving the sample relative to the MR system, e.g. spinning mechanisms, flow cells or means for positioning the sample inside a spectrometer
 
 - 
        
- G—PHYSICS
 - G01—MEASURING; TESTING
 - G01R—MEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
 - G01R33/00—Arrangements or instruments for measuring magnetic variables
 - G01R33/20—Arrangements or instruments for measuring magnetic variables involving magnetic resonance
 - G01R33/60—Arrangements or instruments for measuring magnetic variables involving magnetic resonance using electron paramagnetic resonance
 
 
Definitions
- the present invention concerns detecting and dosing oxygen in an atmosphere to be tested.
 - the invention concerns implementing known methods with the aid of a suitable probe for dosing oxygen by means of electronic paramagnetic resonance spectrometry of the lithium phtalocyanine molecule in its particular quadratic crystalline form.
 - known methods have been described in the documents FR-A-90 08738 and FR-A-90 08739 dated Jul. 10, 1990.
 - the molecular configuration of the quadratic crystalline form of the lithium phtalocyanine enables the latter to solely selectively trap the oxygen molecules 02.
 - the trapped molecule 02 creates a magnetic coupling which affects the electric paramagnetic resonance signal of the phtalocyanine and allows for its spectrometric identification and accordingly for detecting the presence and measuring the quantity of oxygen molecules 02 in a gaseous mixture bathing a sample of lithium phtalocyanine.
 - the phtalocyanines used in the invention are radical-like type phtalocyanines, this special characteristic implying that the width of their electronic paramagnetic resonance line varies almost linearly with the oxygen content in a range of oxygen concentrations of between 0 and 10%, which easily allows a quantitative dosing to be made.
 - the object of the present invention is to provide a probe for detecting and dosing the molecular oxygen by means of electronic resonance spectrometry of the lithium phtalocyanine, thus simply resolving the aforesaid drawbacks whilst being able to be easily applied to industrial applications.
 - At least one fixed glass tube generally having the shape of a hairpin, traversed by a flow of the atmosphere to be tested, at the top of which a chamber with porous walls traversed by said flow contains the phtalocyanine sample and is surrounded by the spires of coil for exciting and detecting the electronic resonance;
 - a movable magnet having a field frame with generally an elongated tubular cylindrical shape whose central pipe possesses a shape and dimensions enabling it to be adapted around the preceding tube which it then covers completely, this movable magnet being provided with windings enabling it to create perpendicular to the field of said excitation coil the continuous field Bo for polarizing the lithium phtalocyanine and the oscillating field for scanning this polarization Bo so as to find the state of resonance.
 - the two main characteristics of the probe-of the invention reside firstly in the fact of carrying out a measurement in a flow of the atmosphere to be tested, the lithium phtalocyanine sample being trapped inside this flow in a chamber with porous walls traversed by this same flow, and secondly as regards the movable design of the scanning and polarization magnet which, by virtue of its shape, can be used as a housing for the glass tube.
 - the chamber with porous walls which formerly was not easy to do, is able to keep in place at a fixed location the phtalocyanine sample whilst enabling the latter to be traversed by the flow of air to be tested.
 - the movable nature of the magnet especially in an industrial installation where it is desired to measure the percentage of oxygen at several locations of a gaseous flow, only uses a single magnet for several glass tubes fixed at various locations of a gaseous path. This results in achieving substantial savings as mentioned earlier since the polarization magnet is a delicate part to produce and thus an extremely expensive one.
 - the chamber with porous walls containing the lithium phtalocyanine sample is made of sintered glass.
 - the two inlet and outlet branches of the glass tube are connected to a solid stainless steel piece comprising a hollow pipe to allow for the flow of the gas constituting the atmosphere to be tested, and two inlet and outlet tubes, also made of stainless steel, are welded to the two branches of the glass tube.
 - This solid stainless steel piece used to bring it from the atmosphere to be tested into the glass tube, is also able to be used with the aid of screws and internal screw threads so as to ensure the accurate fixing of the polarization magnet around the tube as the latter is welded permanently to said piece.
 - the polarization and scanning winding is divided into several sections along the wall of the magnetic frame so that its center of gravity is situated inside the chamber with porous walls and creates a homogeneous field in the entire chamber.
 - FIG. 1 shows the glass tube secured to its solid stainless steel piece
 - FIG. 2 shows the same piece but on this occasion covered with the polarization magnet fixed at its upper portion to the solid stainless steel piece.
 - FIG. 1 shows the glass tube 2 whose general shape is that of a hairpin with one inlet branch 4, one outlet branch 6 and a top 8 where the chamber with porous walls 10 is clearly located. Shown at the lower portion of FIG. 1 is a pip 12 which is used to introduce the lithium phtalocyanine into the chamber 10, after which it it closed permanently.
 - the atmosphere it is desired to test in the glass tube 2 circulates along the direction of the arrows F by traversing the sintered glass walls 14 of the chamber with porous walls.
 - Shown at the upper portion of FIG. 1 is the solid stainless steel piece 16 which is used as a support for the glass tube 4 and, as can be seen on the following FIG. 2, for supporting the polarization magnet.
 - This solid stainless steel piece comprises a hollow pipe 18 for admitting the atmosphere to be tested into the tube 2, as well as a hollow pipe 22 for the outward emission of the flow of said atmosphere.
 - Two tubes, one inlet tube 22 and one outlet tube 24, also form part of the solid piece 16 and are also made of stainless steel. The connection of the tube 2 to these tubes 22 and 24 is effected by welds given on the drawing the references 26 and 28.
 - the coil used for exciting the lithium phtalocyanine and detecting the electronic paramagnetic resonance line is formed of two spires surrounding the chamber with porous walls 10 and visible on the figure at 30 and 32. Once this coil is fixed to the top of the glass tube immediately close to the chamber with porous walls 10, it is a simple matter to excite the lithium phtalocyanine which, for reasons of more clarity, has not been shown in the chamber 10 on FIG. 1.
 - the use of a single coil for excitation and detection has already been described by A. Abragam in "The Principles of Nuclear Magnetism", pages 78 to 80.
 - FIG. 2 shows all the elements of FIG. 1 bearing the same reference numbers.
 - this FIG. 2 corresponds to the situation in which the scanning and polarization magnet 34 is fixed around the glass tube 2 where it is encompassed like a cover.
 - This magnet 34 is fixed to the solid stainless steel piece 16 by a screw and internal screw thread system 36, and at the lower portion of the drawing of FIG. 2, divided into four sections are the scanning and polarization coils 38 for the polarization induction Bo required for triggering the electronic paramagnetic resonance and polarization phenomenon of the lithium phtalocyanine crystals situated at the top of the glass tube 2.
 - This winding 38 is effected split up symmetrically into four sections with respect to the plane XX of FIG. 2 so as to create, as indicated earlier, a magnetic induction as homogeneous as possible in the entire volume of the chamber with porous walls 10.
 - One of the major advantages of the probe of the present invention resides in the fact that, as the scanning and polarization magnet 34 is easily able to be separated from the solid stainless steel piece 16, it is possible to have in an industrial installation several glass tubes comparable to those of FIG. 1 situated at different locations but still able to be used for detection measurements and the dosing of oxygen via the mere fact that they can be adapted to a single polarization magnet 34.
 
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- Physics & Mathematics (AREA)
 - Condensed Matter Physics & Semiconductors (AREA)
 - General Physics & Mathematics (AREA)
 - Investigating Or Analyzing Materials By The Use Of Magnetic Means (AREA)
 - Other Investigation Or Analysis Of Materials By Electrical Means (AREA)
 
Abstract
A probe for detecting and dosing molecular oxygen by the electronic paramagnetic resonance spectrometry of a sample of lithium phthalocyanine in contact with the atmosphere to be tested. The probe includes a fixed glass tube with the shape of a hairpin, traversed by a flow of an atmosphere to be tested. The top of the tube contains a chamber with porous walls traversed by the flow of the atmosphere to be tested. The chamber contains the phthalocyanine sample and is surrounded by the spires of an electronic resonance detector trip coil. A movable magnet surrounds the tube and is provided with windings to create a continuous field for polarizing the phthalocyanine sample.
  Description
The present invention concerns detecting and dosing oxygen in an atmosphere to be tested.
    More particularly, but not exclusively, the invention concerns implementing known methods with the aid of a suitable probe for dosing oxygen by means of electronic paramagnetic resonance spectrometry of the lithium phtalocyanine molecule in its particular quadratic crystalline form. These known methods have been described in the documents FR-A-90 08738 and FR-A-90 08739 dated Jul. 10, 1990.
    Mention shall first of all be made briefly to a population of nuclear or electronic spins being placed to be moved in rotation at a frequency Fo=δBo when they are subjected to a high and continuous magnetic induction Bo,δ being the characteristic gyromagnetic ratio of the substance in question. If in addition this polarized substance is subjected to an adjustable radiofrequency magnetic field having a direction perpendicular to the induction Bo, a resonance phenomenon is observed when this adjustable radiofrequency passes through the value Fo. This state of resonance is expressed by an emission or absorption of energy passing through maximums able to be detected.
    Now, the molecular configuration of the quadratic crystalline form of the lithium phtalocyanine enables the latter to solely selectively trap the oxygen molecules 02. The trapped molecule 02 creates a magnetic coupling which affects the electric paramagnetic resonance signal of the phtalocyanine and allows for its spectrometric identification and accordingly for detecting the presence and measuring the quantity of oxygen molecules 02 in a gaseous mixture bathing a sample of lithium phtalocyanine. Furthermore, the phtalocyanines used in the invention are radical-like type phtalocyanines, this special characteristic implying that the width of their electronic paramagnetic resonance line varies almost linearly with the oxygen content in a range of oxygen concentrations of between 0 and 10%, which easily allows a quantitative dosing to be made.
    The methods for detecting an electronic resonance signal are known to experts in this field and shall therefore not be described further in detail. In the present invention, any known method may be used and in particular the one described in the prior document FR-A-99 09830 dated Jul. 20 1988.
    Nevertheless in theory, the passage through the state of magnetic resonance may be provoked, both by scanning the polarization induction Bo and also by varying the frequency of the excitation field. It is the first method which shall be described in the remainder of this text, but it needs to be understood that this is merely a non-restrictive option.
    Although the principle of the detection of molecular oxygen by means of electronic paramagnetic resonance by lithium phtalocyanine has been known from the documents FR-A-90 08738 and FR-A-90 08739 dated Jul. 10, 1990, no embodiment of an industrial device has occurred since this date owing to the difficulties for designing an operational probe, especially as regards the introduction of the lithium phtalocyanine into the atmosphere to be tested, this introduction needing to be compatible with the possibility of precisely subjecting it to the magnetic inductions required for the production and detection of the electronic paramagnetic resonance phenomenon. Now, it is well known that the magnets and coils used for these purposes are extremely delicate to embody and are generally extremely expensive.
    The object of the present invention is to provide a probe for detecting and dosing the molecular oxygen by means of electronic resonance spectrometry of the lithium phtalocyanine, thus simply resolving the aforesaid drawbacks whilst being able to be easily applied to industrial applications.
    This probe is characterized in that it includes:
    at least one fixed glass tube, generally having the shape of a hairpin, traversed by a flow of the atmosphere to be tested, at the top of which a chamber with porous walls traversed by said flow contains the phtalocyanine sample and is surrounded by the spires of coil for exciting and detecting the electronic resonance;
    a movable magnet having a field frame with generally an elongated tubular cylindrical shape whose central pipe possesses a shape and dimensions enabling it to be adapted around the preceding tube which it then covers completely, this movable magnet being provided with windings enabling it to create perpendicular to the field of said excitation coil the continuous field Bo for polarizing the lithium phtalocyanine and the oscillating field for scanning this polarization Bo so as to find the state of resonance.
    According to the preceding definition, the two main characteristics of the probe-of the invention reside firstly in the fact of carrying out a measurement in a flow of the atmosphere to be tested, the lithium phtalocyanine sample being trapped inside this flow in a chamber with porous walls traversed by this same flow, and secondly as regards the movable design of the scanning and polarization magnet which, by virtue of its shape, can be used as a housing for the glass tube. The chamber with porous walls, which formerly was not easy to do, is able to keep in place at a fixed location the phtalocyanine sample whilst enabling the latter to be traversed by the flow of air to be tested. Moreover, the movable nature of the magnet, especially in an industrial installation where it is desired to measure the percentage of oxygen at several locations of a gaseous flow, only uses a single magnet for several glass tubes fixed at various locations of a gaseous path. This results in achieving substantial savings as mentioned earlier since the polarization magnet is a delicate part to produce and thus an extremely expensive one.
    According to one particularly advantageous embodiment of the invention, the chamber with porous walls containing the lithium phtalocyanine sample is made of sintered glass.
    According to another advantageous embodiment of the invention, the two inlet and outlet branches of the glass tube are connected to a solid stainless steel piece comprising a hollow pipe to allow for the flow of the gas constituting the atmosphere to be tested, and two inlet and outlet tubes, also made of stainless steel, are welded to the two branches of the glass tube. This solid stainless steel piece, used to bring it from the atmosphere to be tested into the glass tube, is also able to be used with the aid of screws and internal screw threads so as to ensure the accurate fixing of the polarization magnet around the tube as the latter is welded permanently to said piece.
    Finally, according to another advantageous characteristic of the present invention, the polarization and scanning winding is divided into several sections along the wall of the magnetic frame so that its center of gravity is situated inside the chamber with porous walls and creates a homogeneous field in the entire chamber.
    This disposition allows for considerable flexibility in establishing the scanning and polarization magnetic induction, since it is the distribution of the spires of the coil in the various sections of the wall of the magnetic frame which makes it possible at the exact desired location to obtain a homogeneous field concerning a dimension equal at least to that of the chamber with porous walls containing the phtalocyanine. The shapes and dimensions of these coils may be deduced from the article by L. B. Lugansky entitled "On Optical Synthesis of Magnetic Fields" in Journal of Physics, 1, 53 (1990).
    
    
    The present invention shall be more readily understood from a reading of the following non-restrictive example of a description of the probe of the invention given solely by way of illustration with reference to the accompanying figures on which:
    FIG. 1 shows the glass tube secured to its solid stainless steel piece;
    FIG. 2 shows the same piece but on this occasion covered with the polarization magnet fixed at its upper portion to the solid stainless steel piece.
    
    
    FIG. 1 shows the glass tube 2 whose general shape is that of a hairpin with one inlet branch 4, one outlet branch  6 and a top 8 where the chamber with porous walls  10 is clearly located. Shown at the lower portion of FIG. 1 is a pip  12 which is used to introduce the lithium phtalocyanine into the chamber  10, after which it it closed permanently.
    The atmosphere it is desired to test in the glass tube 2 circulates along the direction of the arrows F by traversing the sintered glass walls  14 of the chamber with porous walls. Shown at the upper portion of FIG. 1 is the solid stainless steel piece  16 which is used as a support for the glass tube 4 and, as can be seen on the following FIG. 2, for supporting the polarization magnet. This solid stainless steel piece comprises a hollow pipe  18 for admitting the atmosphere to be tested into the tube 2, as well as a hollow pipe  22 for the outward emission of the flow of said atmosphere. Two tubes, one inlet tube  22 and one outlet tube  24, also form part of the solid piece  16 and are also made of stainless steel. The connection of the tube 2 to these  tubes    22 and 24 is effected by welds given on the drawing the  references    26 and 28.
    Finally, the coil used for exciting the lithium phtalocyanine and detecting the electronic paramagnetic resonance line is formed of two spires surrounding the chamber with porous walls  10 and visible on the figure at 30 and 32. Once this coil is fixed to the top of the glass tube immediately close to the chamber with porous walls  10, it is a simple matter to excite the lithium phtalocyanine which, for reasons of more clarity, has not been shown in the chamber  10 on FIG. 1. The use of a single coil for excitation and detection has already been described by A. Abragam in "The Principles of Nuclear Magnetism", pages 78 to 80.
    FIG. 2 shows all the elements of FIG. 1 bearing the same reference numbers. However, this FIG. 2 corresponds to the situation in which the scanning and polarization magnet  34 is fixed around the glass tube 2 where it is encompassed like a cover. This magnet  34 is fixed to the solid stainless steel piece  16 by a screw and internal screw thread system  36, and at the lower portion of the drawing of FIG. 2, divided into four sections are the scanning and polarization coils  38 for the polarization induction Bo required for triggering the electronic paramagnetic resonance and polarization phenomenon of the lithium phtalocyanine crystals situated at the top of the glass tube 2. This winding  38 is effected split up symmetrically into four sections with respect to the plane XX of FIG. 2 so as to create, as indicated earlier, a magnetic induction as homogeneous as possible in the entire volume of the chamber with porous walls  10.
    One of the major advantages of the probe of the present invention resides in the fact that, as the scanning and polarization magnet  34 is easily able to be separated from the solid stainless steel piece  16, it is possible to have in an industrial installation several glass tubes comparable to those of FIG. 1 situated at different locations but still able to be used for detection measurements and the dosing of oxygen via the mere fact that they can be adapted to a single polarization magnet  34.
    
  Claims (7)
1. A probe for detecting the concentration of molecular oxygen in an atmosphere comprising:
    a) at least one glass tube having a top, an inlet branch, and an outlet branch, said tube having the general shape of a hairpin, the top of said tube having a chamber with porous walls, said chamber containing a lithium phthalocyanine sample;
 b) excitation coil means for providing an excitation magnetic field in said chamber and for detecting an electronic paramagnetic resonance signal from said lithium phthalocyanine; and
 c) a movable magnet for generating a magnetic field Bo in said chamber for polarizing the lithium phthalocyanine.
 2. The probe according to claim 1, wherein
    (i) said excitation coil means comprises a coil surrounding said chamber;
 (ii) said movable magnet has a generally elongated cylindrical tubular shape; and
 (iii) said probe further comprises a means for attaching said movable magnet to said tube.
 3. The probe according to claim 1, wherein said movable magnet completely surrounds said tube when said means for attaching said movable magnet to said tube attaches said movable magnet to said tube.
    4. Probe according to claim 1, wherein the chamber with porous walls containing the lithium phtalocyanine sample is made of sintered glass.
    5. A probe according to claim 1, wherein said movable magnet comprises scanning and polarization windings that are divided into several sections along a wall of the movable magnet so that a center of gravity of the scanning and polarization windings is situated inside the chamber with porous walls and creates a homogenous field in the chamber.
    6. Probe according to claim 1 or 4, wherein the scanning and polarization winding is divided into several sections along the wall of the magnetic frame so that its center of gravity is situated inside the chamber with porous walls and creates a homogeneous field in the entire chamber.
    7. The probe according to claim 1 or 4, further comprising a stainless steel piece having an inlet, an outlet, and a chamber, said steel piece inlet and outlet being fixedly attached to said tube inlet branch and outlet branch, respectively, so that said atmosphere can flow continuously from said steel piece through said tube and back to said steel piece.
    Applications Claiming Priority (2)
| Application Number | Priority Date | Filing Date | Title | 
|---|---|---|---|
| FR9211203 | 1992-09-21 | ||
| FR9211203A FR2696008B1 (en) | 1992-09-21 | 1992-09-21 | Probe for detection and determination of molecular oxygen by electronic paramagnetic resonance spectrometry. | 
Publications (1)
| Publication Number | Publication Date | 
|---|---|
| US5504429A true US5504429A (en) | 1996-04-02 | 
Family
ID=9433692
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date | 
|---|---|---|---|
| US08/114,837 Expired - Fee Related US5504429A (en) | 1992-09-21 | 1993-09-02 | Probe for detecting and dosing molecular oxygen by means of electronic paramagnetic resonance spectrometry | 
Country Status (4)
| Country | Link | 
|---|---|
| US (1) | US5504429A (en) | 
| EP (1) | EP0589756B1 (en) | 
| DE (1) | DE69313393D1 (en) | 
| FR (1) | FR2696008B1 (en) | 
Families Citing this family (4)
| Publication number | Priority date | Publication date | Assignee | Title | 
|---|---|---|---|---|
| FR2696008B1 (en) * | 1992-09-21 | 1994-11-04 | Commissariat Energie Atomique | Probe for detection and determination of molecular oxygen by electronic paramagnetic resonance spectrometry. | 
| CN103018269B (en) * | 2013-01-05 | 2017-09-12 | 中国人民解放军军事医学科学院放射与辐射医学研究所 | A kind of rectangle electron paramagnetic resonance probe of chamber external pelivimetry sample | 
| CN103033526B (en) * | 2013-01-05 | 2017-09-12 | 中国人民解放军军事医学科学院放射与辐射医学研究所 | A kind of cylindrical electron paramagnetic resonance probe of external sample measurement | 
| CN107107362B (en) | 2014-12-22 | 2020-08-04 | 比克-维尔莱克 | razor blade | 
Citations (8)
| Publication number | Priority date | Publication date | Assignee | Title | 
|---|---|---|---|---|
| US4593248A (en) * | 1984-03-27 | 1986-06-03 | The Medical College Of Wisconsin, Inc. | Oxymeter | 
| US4803624A (en) * | 1986-09-19 | 1989-02-07 | Pilbrow John R | Electron spin resonance spectrometer | 
| EP0467748A1 (en) * | 1990-07-10 | 1992-01-22 | Commissariat A L'energie Atomique | Method for detection or dosage of oxygen by EPR spectrometry using lithium phthalocyanine radicals and composition usable for in-vivo dosage | 
| US5112597A (en) * | 1990-07-10 | 1992-05-12 | Commissariat A L'energie Atomique | Radical lithium phthalocyanine crystals, their preparation process and their use for the in vivo determination of molecular oxygen | 
| US5159269A (en) * | 1989-06-14 | 1992-10-27 | Commissariat A L'energie Atomique | Process for the preparation of a radical cation salt and its use in an electron paramagnetic resonance (epr) magnetometer | 
| EP0589756A1 (en) * | 1992-09-21 | 1994-03-30 | Commissariat A L'energie Atomique | Probe for detection and dosage of molecular oxygen by EPR spectrometry | 
| US5313162A (en) * | 1991-04-27 | 1994-05-17 | Forschungszentrum Julich Gmbh | Apparatus for throughflow NMR spectroscopy, especially for cell suspensions | 
| US5347219A (en) * | 1991-08-02 | 1994-09-13 | Bruker Analytische Messtechnik Gmbh | Resonator arrangement for electron spin resonance spectroscopy | 
- 
        1992
        
- 1992-09-21 FR FR9211203A patent/FR2696008B1/en not_active Expired - Fee Related
 
 - 
        1993
        
- 1993-09-02 US US08/114,837 patent/US5504429A/en not_active Expired - Fee Related
 - 1993-09-16 DE DE69313393T patent/DE69313393D1/en not_active Expired - Lifetime
 - 1993-09-16 EP EP93402254A patent/EP0589756B1/en not_active Expired - Lifetime
 
 
Patent Citations (9)
| Publication number | Priority date | Publication date | Assignee | Title | 
|---|---|---|---|---|
| US4593248A (en) * | 1984-03-27 | 1986-06-03 | The Medical College Of Wisconsin, Inc. | Oxymeter | 
| US4803624A (en) * | 1986-09-19 | 1989-02-07 | Pilbrow John R | Electron spin resonance spectrometer | 
| US5159269A (en) * | 1989-06-14 | 1992-10-27 | Commissariat A L'energie Atomique | Process for the preparation of a radical cation salt and its use in an electron paramagnetic resonance (epr) magnetometer | 
| EP0467748A1 (en) * | 1990-07-10 | 1992-01-22 | Commissariat A L'energie Atomique | Method for detection or dosage of oxygen by EPR spectrometry using lithium phthalocyanine radicals and composition usable for in-vivo dosage | 
| US5112597A (en) * | 1990-07-10 | 1992-05-12 | Commissariat A L'energie Atomique | Radical lithium phthalocyanine crystals, their preparation process and their use for the in vivo determination of molecular oxygen | 
| US5258313A (en) * | 1990-07-10 | 1993-11-02 | Commissariat A L'energie Atomique | Process for the detection or determination of oxygen by EPR spectrometry using radical lithium phthalocyanines and composition usable for in vivo determination | 
| US5313162A (en) * | 1991-04-27 | 1994-05-17 | Forschungszentrum Julich Gmbh | Apparatus for throughflow NMR spectroscopy, especially for cell suspensions | 
| US5347219A (en) * | 1991-08-02 | 1994-09-13 | Bruker Analytische Messtechnik Gmbh | Resonator arrangement for electron spin resonance spectroscopy | 
| EP0589756A1 (en) * | 1992-09-21 | 1994-03-30 | Commissariat A L'energie Atomique | Probe for detection and dosage of molecular oxygen by EPR spectrometry | 
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| Title | 
|---|
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| Magnetic Resonance in Medicine, vol. 20, No. 2, Aug. 1, 1991, pp. 333-339, H. M. Swartz, et al., "Measurements of Pertinent Concentrations of Oxygen in Vivo". | 
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| Sensors and Actuators B, vol. B6, No. 1-3, Jan. 1, 1992, pp. 266-269, D. Duret, et al., "Oxygen Concentration Measurements Using the ESR Line Modification of PcLi Molecules". | 
| Synthetic Metals, vol. 52, No. 1, Sep. 15, 1992, pp. 57 69, F. Bensebaa, et al., The Effect of Oxygen on Phthalocyanine Radicals II. Comparative Study of Two Lithium Phthalocyanine Powder Derivates by Continuous and Pulsed ESR . * | 
| Synthetic Metals, vol. 52, No. 1, Sep. 15, 1992, pp. 57-69, F. Bensebaa, et al., "The Effect of Oxygen on Phthalocyanine Radicals II. Comparative Study of Two Lithium Phthalocyanine Powder Derivates by Continuous and Pulsed ESR". | 
Also Published As
| Publication number | Publication date | 
|---|---|
| DE69313393D1 (en) | 1997-10-02 | 
| EP0589756A1 (en) | 1994-03-30 | 
| EP0589756B1 (en) | 1997-08-27 | 
| FR2696008B1 (en) | 1994-11-04 | 
| FR2696008A1 (en) | 1994-03-25 | 
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